JPH0222505A - Laser interference measuring instrument - Google Patents

Laser interference measuring instrument

Info

Publication number
JPH0222505A
JPH0222505A JP17227888A JP17227888A JPH0222505A JP H0222505 A JPH0222505 A JP H0222505A JP 17227888 A JP17227888 A JP 17227888A JP 17227888 A JP17227888 A JP 17227888A JP H0222505 A JPH0222505 A JP H0222505A
Authority
JP
Japan
Prior art keywords
magnification
light
low
measured
image
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP17227888A
Other languages
Japanese (ja)
Inventor
Yojiro Iwamoto
岩本 洋次郎
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tokyo Seimitsu Co Ltd
Original Assignee
Tokyo Seimitsu Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tokyo Seimitsu Co Ltd filed Critical Tokyo Seimitsu Co Ltd
Priority to JP17227888A priority Critical patent/JPH0222505A/en
Publication of JPH0222505A publication Critical patent/JPH0222505A/en
Pending legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)

Abstract

PURPOSE:To accurately measure the shape of a fine part by picking up an image of a measured surface with low magnification and high magnification under the same conditions. CONSTITUTION:The light beam emitted by a laser light source 10 is changed in direction by 90 deg. through a mirror 12 and the made into parallel luminous flux by a beam expander 14 to be made incident on a half-mirror 16. This light beam is changed in direction by 90 deg. and the light is emitted on the surface 18 to be measured and also emitted on a reference surface 20. The reflected light beams from the surface 18 to be measured and reference surface 20 are made incident on a low-magnification image forming lens 26 through a beam splitter 24. Further, the light beam which is reflected by the splitter 24 is made incident on a high-magnification image forming lens 30 as interference light. Further, a camera 28 for low-magnification measurement picks up an image of interference fringes corresponding to the low magnification and sends its image signal to a memory 34. Further, a camera 32 for the high magnification picks up an image of interference fringes corresponding to the high magnification and sends its image signal to a memory 40. Thus, the shape of the fine part is accurately measured.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はレーザ干渉測定装置に係り、特に低倍率観測用
光学系と高倍率観測用光学系を備えたレーザ干渉測定装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a laser interference measurement device, and more particularly to a laser interference measurement device equipped with an optical system for low magnification observation and an optical system for high magnification observation.

〔従来の技術〕[Conventional technology]

従来、レーザ光を測定鏡と参照鏡とに照射すると共に、
その反射光を干渉させ、この干渉光の干渉縞の強弱から
被測定物の表面形状(表面の凹凸の度合)を測定するレ
ーザ干渉測定装置が知られている。
Conventionally, while irradiating a measurement mirror and a reference mirror with laser light,
A laser interference measurement device is known that interferes with the reflected light and measures the surface shape (degree of surface irregularity) of the object to be measured from the intensity of interference fringes of the interference light.

また、このようなレーザ干渉測定装置において、低倍率
観測用光学系と高倍率観測用光学系とを備えたレーザ干
渉測定装置も知られている。このような低倍率観測用光
学系と高倍率観測用光学系を備えたレーザ干渉測定装置
は、ズーム光学系によって倍率を切換えるタイプと、複
数の対物レンズを備え、この対物レンズを交換レンズ方
式によって倍率を変えるものとがある。このような倍率
切換機構を持ったレーザ干渉測定装置は、先ず最初に低
倍率光学系で測定面を観察し、その後高倍率光学系に切
換えて必要な微細部分を高倍率で測定するようにしてい
る。
Furthermore, among such laser interference measurement devices, a laser interference measurement device including a low-magnification observation optical system and a high-magnification observation optical system is also known. Laser interference measurement equipment equipped with such a low-magnification observation optical system and a high-magnification observation optical system is of the type that uses a zoom optical system to switch the magnification, and has multiple objective lenses, which can be exchanged using an interchangeable lens system. There are some that change the magnification. A laser interferometer with such a magnification switching mechanism first observes the surface to be measured using a low-magnification optical system, and then switches to a high-magnification optical system to measure the required minute part at high magnification. There is.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

しかしながら、前記従来の倍率切換機構を持ったレーザ
干渉測定装置では、低倍率光学系で観測した時点と高倍
率光学系で観測した時点とは時間が経過してふり、同一
の条件で観測されていない虞がある。例えば、このよう
なレーザ干渉測定装置の観察は撮像カメラにより行われ
るのであるが、拡大観測した場合、測定面の表面形状に
よる干渉縞の明暗であるのか、時間経過に伴うワークの
傾き、空気のゆらぎ等の影響の干渉縞の明暗なのか時間
が経過しているので判断できないため、低倍率で測定し
た表面形状に対する高倍率で測定した表面形状の相対的
な傾斜及び相対的な高さが測定できない等の不具合があ
る。このような現象は特に磁気ヘッドの表面形状測定に
用いられる1/100μmオーダの測定を行う場合に生
じてくる。
However, in the conventional laser interferometer with a magnification switching mechanism, time has elapsed between the time of observation with the low-magnification optical system and the time of observation with the high-magnification optical system, and the observations are not made under the same conditions. There is a possibility that it will not happen. For example, observation of such a laser interference measurement device is performed using an imaging camera, but when observed under magnification, the brightness and darkness of the interference fringes may be due to the surface shape of the measurement surface, the tilt of the workpiece over time, or the presence of air. Since it is impossible to determine whether the brightness or darkness of the interference fringes is due to the effects of fluctuations etc. as time has passed, the relative inclination and relative height of the surface shape measured at high magnification with respect to the surface shape measured at low magnification are measured. There are some problems such as not being able to do it. Such a phenomenon occurs particularly when measuring on the order of 1/100 μm, which is used to measure the surface shape of a magnetic head.

本発明はこのような事情に鑑みてなされたもので、同一
の条件で低倍率光学系と高倍率光学系とで観測できるレ
ーザ干渉測定装置を提案することを目的としている。
The present invention has been made in view of these circumstances, and it is an object of the present invention to propose a laser interference measurement device that can perform observation using a low-magnification optical system and a high-magnification optical system under the same conditions.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、レーザ光を測定鏡と参照鏡とに照射すると共
にその反射光を干渉させ、この干渉光の干渉縞の強弱か
ら被測定物の表面形状を測定するレーザ干渉測定装置に
於いて、干渉光を2方光に分けるビームスプリッタを設
け、分光した光の一方を撮像カメラを含む低倍率撮像光
学系に導くと共に、他方の光を撮像カメラを含む高倍率
撮像光学系に導き、夫々の撮像カメラからの画像信号を
記憶するメモリ手段を設けると共に低倍率で撮像した画
像と高倍率で撮像した画像を表示する表示手段を設けた
ことを特徴としている。
The present invention provides a laser interference measurement device that irradiates a measurement mirror and a reference mirror with a laser beam, causes the reflected light to interfere with each other, and measures the surface shape of a workpiece based on the intensity of interference fringes of this interference light. A beam splitter is provided to separate the interference light into two beams, and one of the separated lights is guided to a low-magnification imaging optical system including an imaging camera, and the other light is guided to a high-magnification imaging optical system including an imaging camera. The present invention is characterized in that it is provided with a memory means for storing an image signal from an imaging camera and a display means for displaying an image taken at a low magnification and an image taken at a high magnification.

〔作用〕[Effect]

本発明に係るレーザ干渉測定装置においては、干渉縞を
低倍率光学系と高倍率光学系との両方で同時に観測する
ことができる。従って、先ず低倍率光学系で撮像してそ
の表面形状等の画像信号をメモリ手段に記憶し、同時に
高倍率光学系で撮像してその画像信号をメモリ手段で記
録し、その後、低倍率光学系で撮像した形状と高倍率光
学系で撮像した形状の両方をCRT画面又はプリンタで
表示する。この結果、同一の条件で低倍率と高倍率との
両方で観測することができる。
In the laser interference measurement device according to the present invention, interference fringes can be observed simultaneously using both the low-magnification optical system and the high-magnification optical system. Therefore, first, an image is taken with a low magnification optical system and an image signal such as the surface shape is stored in a memory means, and at the same time an image is taken with a high magnification optical system and the image signal is recorded in a memory means. Both the shape imaged by the camera and the shape imaged by the high-magnification optical system are displayed on a CRT screen or a printer. As a result, it is possible to observe at both low magnification and high magnification under the same conditions.

〔実施例〕〔Example〕

以下添付図面に従って本発明に係るレーザ干渉測定装置
の好ましい実施例を詳説する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Preferred embodiments of the laser interference measurement apparatus according to the present invention will be described in detail below with reference to the accompanying drawings.

第1図は本発明に係るレーザ干渉測定装置を用いて面形
状を測定する場合の装置の構造が示され、lOはレーザ
光源、12はミラー 14はビームエキスパンダ、16
はハーフミラ−である。更に、18は被測定面、20は
参照面、22はピエゾ素子、24はビームスプリフタ、
26は低倍率用結像レンズ、28は低倍率測定用カメラ
、30は高倍率用結像レンズ、32は高倍率測定用カメ
ラである。カメラ28で撮像した画像信号はメモリ34
で記録され、コンピュータ36で画像処理されたのちC
RT画面38又はプリンタ等により表示されるようにな
っている。更に、高倍率測定用カメラ32で撮像された
画像信号はメモリ40で記録され、コンビ異−夕36で
画像処理されたのち、CRT画面38又はプリンタによ
り表示されるようになっている。
FIG. 1 shows the structure of a device for measuring a surface shape using a laser interference measuring device according to the present invention, in which lO is a laser light source, 12 is a mirror, 14 is a beam expander, and 16
is a half mirror. Further, 18 is a surface to be measured, 20 is a reference surface, 22 is a piezo element, 24 is a beam splitter,
26 is an imaging lens for low magnification, 28 is a camera for low magnification measurement, 30 is an imaging lens for high magnification, and 32 is a camera for high magnification measurement. The image signal captured by the camera 28 is stored in the memory 34
After being recorded in C and image processed by computer
It is designed to be displayed on the RT screen 38 or on a printer or the like. Furthermore, the image signal taken by the high-magnification measuring camera 32 is recorded in a memory 40, subjected to image processing by a combination camera 36, and then displayed on a CRT screen 38 or a printer.

前記の如く構成されたレーザ干渉測定装置において、レ
ーザ光源lOから出射した光はミラー12で90°方向
変換されたのち、ビームエキスパンダ14で平行光束と
され、その後ハーフミラ−16に入射する。ハーフミラ
−16に入射した光は90°方向を変えられ、被測定面
18に向けて出射すると共に参照面20に向けて出射す
る。被測定面18と参照面20からの反射光はビームス
プリッタ24を通過して干渉光として低倍率用結像レン
ズ26に入射する。一方、ビームスプリッタ24で反射
された光は干渉光として高倍率用結像レンズ30に入射
する。低倍率測定用カメラ28では低倍率における干渉
縞が撮像され、その画像信号がメモリ34に送られる。
In the laser interference measurement apparatus configured as described above, the light emitted from the laser light source 1O is converted into a parallel light beam by the beam expander 14 after being changed in direction by 90 degrees by the mirror 12, and then enters the half mirror 16. The direction of the light incident on the half mirror 16 is changed by 90°, and the light is emitted toward the measurement surface 18 and the reference surface 20 . The reflected light from the measurement surface 18 and the reference surface 20 passes through the beam splitter 24 and enters the low-magnification imaging lens 26 as interference light. On the other hand, the light reflected by the beam splitter 24 enters the high magnification imaging lens 30 as interference light. The low magnification measurement camera 28 captures an image of interference fringes at low magnification, and the image signal is sent to the memory 34 .

また、高倍率測定用カメラ32では特定部分の高倍率の
干渉縞が撮像され、その画像信号がメモリ40に送られ
る。
Furthermore, the high-magnification measurement camera 32 captures a high-magnification interference fringe image of a specific portion, and the image signal is sent to the memory 40 .

従って、例えばCRT画面38にはコンビニ−タグラフ
イックの技術を用いて低倍率における立体図形Pと同一
条件での高倍率における微小部分の立体図形Qが第2図
に示すように表示されるようになる。
Therefore, for example, on the CRT screen 38, a three-dimensional figure P at a low magnification and a minute three-dimensional figure Q at a high magnification under the same conditions are displayed as shown in FIG. 2 using convenience store graphic technology. Become.

第2図では、干渉縞に基づいて立体図形を表示したので
あるが、これに限定されるものでなく干渉縞を直接表示
するようにしてもよい。
In FIG. 2, a three-dimensional figure is displayed based on interference fringes, but the present invention is not limited to this, and interference fringes may be directly displayed.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明に係るレーザ干渉側装置によ
れば、測定面を低倍率と高倍率とで同一条件で撮像する
ことができるので、正確に微細部分の形状等を測定する
ことができる。
As explained above, according to the laser interference side device according to the present invention, it is possible to image the measurement surface under the same conditions at low magnification and high magnification, so it is possible to accurately measure the shape etc. of minute parts. .

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明に係るレーザ干渉測定装置の構造を示す
説明図、第2図は本発明に係るレーザ干渉測定装置で観
測した表面形状の立体図を示す説明図である。 10・・・レーザ光源、 18・・・被測定面、 20
・・・参照面、 28・・・低倍率測定用カメラ、  
32・・・高倍率測定用カメラ、  34.40・・・
メモリ、38・・・CRT画面。 !、事件の表示 20発明の名称 3、補正をする者 事件との関係 住     所 名      称 4、代理人 住 所 手続補正書 昭和63年特許願第172278号 レーザ干渉測定装置
FIG. 1 is an explanatory diagram showing the structure of a laser interference measurement device according to the present invention, and FIG. 2 is an explanatory diagram showing a three-dimensional view of a surface shape observed by the laser interference measurement device according to the invention. 10... Laser light source, 18... Surface to be measured, 20
...Reference plane, 28...Low magnification measurement camera,
32...High magnification measurement camera, 34.40...
Memory, 38...CRT screen. ! , Indication of the case 20 Title of the invention 3 Address of the person making the amendment Name 4 Name of the address of the agent Procedural amendment 1986 Patent application No. 172278 Laser interference measurement device

Claims (1)

【特許請求の範囲】[Claims] (1)レーザ光を被測定面と参照鏡とに照射すると共に
その反射光を干渉させ、この干渉光の干渉縞の強弱から
被測定物の表面形状を測定するレーザ干渉測定装置に於
いて、 干渉光を2方光に分けるビームスプリッタを設け、分光
した光の一方を撮像カメラを含む低倍率撮像光学系に導
くと共に、他方の光を撮像カメラを含む高倍率撮像光学
系に導き、夫々の撮像カメラからの画像信号を記憶する
メモリ手段を設けると共に低倍率で撮像した画像と高倍
率で撮像した画像を表示する表示手段を設けたことを特
徴とするレーザ干渉測定装置。
(1) In a laser interference measurement device that irradiates a surface to be measured and a reference mirror with a laser beam and causes the reflected light to interfere with each other, the surface shape of the object to be measured is measured from the intensity of interference fringes of this interference light. A beam splitter is provided to separate the interference light into two beams, and one of the separated lights is guided to a low-magnification imaging optical system including an imaging camera, and the other light is guided to a high-magnification imaging optical system including an imaging camera. 1. A laser interference measurement device comprising: a memory means for storing an image signal from an imaging camera; and a display means for displaying an image taken at a low magnification and an image taken at a high magnification.
JP17227888A 1988-07-11 1988-07-11 Laser interference measuring instrument Pending JPH0222505A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17227888A JPH0222505A (en) 1988-07-11 1988-07-11 Laser interference measuring instrument

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17227888A JPH0222505A (en) 1988-07-11 1988-07-11 Laser interference measuring instrument

Publications (1)

Publication Number Publication Date
JPH0222505A true JPH0222505A (en) 1990-01-25

Family

ID=15938952

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17227888A Pending JPH0222505A (en) 1988-07-11 1988-07-11 Laser interference measuring instrument

Country Status (1)

Country Link
JP (1) JPH0222505A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2813946A1 (en) 2000-09-11 2002-03-15 Koito Mfg Co Ltd VEHICLE LAMP
US6619825B2 (en) 2000-09-18 2003-09-16 Koito Manufacturing Co., Ltd. Vehicle lamp
JP2009229234A (en) * 2008-03-21 2009-10-08 Fujinon Corp Lightwave interference measuring instrument
JP2009229235A (en) * 2008-03-21 2009-10-08 Fujinon Corp Interference fringe imaging device and lightwave interference measuring instrument equipped therewith
JP2011220816A (en) * 2010-04-09 2011-11-04 Niigata Univ Method for measuring shape of cylindrical surface

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2813946A1 (en) 2000-09-11 2002-03-15 Koito Mfg Co Ltd VEHICLE LAMP
US6619825B2 (en) 2000-09-18 2003-09-16 Koito Manufacturing Co., Ltd. Vehicle lamp
JP2009229234A (en) * 2008-03-21 2009-10-08 Fujinon Corp Lightwave interference measuring instrument
JP2009229235A (en) * 2008-03-21 2009-10-08 Fujinon Corp Interference fringe imaging device and lightwave interference measuring instrument equipped therewith
JP2011220816A (en) * 2010-04-09 2011-11-04 Niigata Univ Method for measuring shape of cylindrical surface

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